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At least 595 records · Page 33

Materials Data on Sr3Bi2 by Materials Project

Sr3BiBi is High-temperature superconductor-like structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional and consists of one bismuth molecule and one Sr3Bi framework. In the Sr3Bi framework, Sr is bonded in a linear geometry to two equivalent Bi atoms. Both Sr–Bi bond lengths are 3.12 Å. Bi is bonded to six equivalent Sr atoms to form corner-sharing BiSr6 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on Ca3Bi2 by Materials Project

Ca3Bi2 is High-temperature superconductor-like structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional and consists of one bismuth molecule and one Ca3Bi framework. In the Ca3Bi framework, Ca is bonded in a linear geometry to two equivalent Bi atoms. Both Ca–Bi bond lengths are 2.94 Å. Bi is bonded to six equivalent Ca atoms to form corner-sharing BiCa6 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on Ba3Bi2 by Materials Project

Ba3BiBi is High-temperature superconductor-like structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional and consists of one bismuth molecule and one Ba3Bi framework. In the Ba3Bi framework, Ba is bonded in a linear geometry to two equivalent Bi atoms. Both Ba–Bi bond lengths are 3.31 Å. Bi is bonded to six equivalent Ba atoms to form corner-sharing BiBa6 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on CaZrF6 by Materials Project

CaZrF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ca2+ is bonded to six equivalent F1- atoms to form CaF6 octahedra that share corners with six equivalent ZrF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ca–F bond lengths are 2.27 Å. Zr4+ is bonded to six equivalent F1- atoms to form ZrF6 octahedra that share corners with six equivalent CaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Zr–F bond lengths are 2.04 Å. F1- is bonded in a linear geometry to one Ca2+ and one Zr4+ atom.

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Materials Data on Sc(NF2)3 by Materials Project

ScNF6N2 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight ammonia molecules and one ScNF6 framework. In the ScNF6 framework, Sc3+ is bonded to six equivalent F1- atoms to form ScF6 octahedra that share corners with six equivalent NF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sc–F bond lengths are 2.07 Å. N1+ is bonded to six equivalent F1- atoms to form NF6 octahedra that share corners with six equivalent ScF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All N–F bond lengths are 1.84 Å. F1- is bonded in a linear geometry to one Sc3+ and one N1+ atom.

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Materials Data on NaVH8(NF3)2 by Materials Project

(NH4)2NaVF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight ammonium molecules and one NaVF6 framework. In the NaVF6 framework, Na1+ is bonded to six equivalent F1- atoms to form NaF6 octahedra that share corners with six equivalent VF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–F bond lengths are 2.29 Å. V3+ is bonded to six equivalent F1- atoms to form VF6 octahedra that share corners with six equivalent NaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All V–F bond lengths are 2.00 Å. F1- is bonded in a linear geometry to one Na1+ and one V3+ atom.

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Materials Data on K3TlI6 by Materials Project

(K)2KTlI6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one KTlI6 framework. In the KTlI6 framework, K1+ is bonded to six equivalent I1- atoms to form KI6 octahedra that share corners with six equivalent TlI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All K–I bond lengths are 3.35 Å. Tl3+ is bonded to six equivalent I1- atoms to form TlI6 octahedra that share corners with six equivalent KI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–I bond lengths are 3.01 Å. I1- is bonded in a linear geometry to one K1+ and one Tl3+ atom.

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Materials Data on K3EuCl6 by Materials Project

(K)2KEuCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one KEuCl6 framework. In the KEuCl6 framework, K1+ is bonded to six equivalent Cl1- atoms to form KCl6 octahedra that share corners with six equivalent EuCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All K–Cl bond lengths are 2.98 Å. Eu3+ is bonded to six equivalent Cl1- atoms to form EuCl6 octahedra that share corners with six equivalent KCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Eu–Cl bond lengths are 2.70 Å. Cl1- is bonded in a linear geometry to one K1+ and one Eu3+ atom.

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Materials Data on WO3 by Materials Project

WO3 is High-temperature superconductor-like structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent W6+ sites. In the first W6+ site, W6+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedra tilt angles range from 4–10°. There are a spread of W–O bond distances ranging from 1.85–2.04 Å. In the second W6+ site, W6+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedra tilt angles range from 4–10°. There are a spread of W–O bond distances ranging from 1.85–2.04 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the fifth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the sixth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the seventh O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the eighth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the ninth O2- site, O2- is bonded in a linear geometry to two W6+ atoms. There is one shorter (1.87 Å) and one longer (2.00 Å) O–W bond length. In the tenth O2- site, O2- is bonded in a linear geometry to two W6+ atoms. There is one shorter (1.88 Å) and one longer (2.00 Å) O–W bond length. In the eleventh O2- site, O2- is bonded in a linear geometry to two W6+ atoms. In the twelfth O2- site, O2- is bonded in a linear geometry to two W6+ atoms.

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Materials Data on Li2CuSbCl6 by Materials Project

(Li)2CuSbCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight lithium molecules and one CuSbCl6 framework. In the CuSbCl6 framework, Cu1+ is bonded to six equivalent Cl1- atoms to form CuCl6 octahedra that share corners with six equivalent SbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cu–Cl bond lengths are 2.46 Å. Sb3+ is bonded to six equivalent Cl1- atoms to form SbCl6 octahedra that share corners with six equivalent CuCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Cl bond lengths are 2.65 Å. Cl1- is bonded in a linear geometry to one Cu1+ and one Sb3+ atom.

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Materials Data on Na3DyCl6 by Materials Project

(Na)2NaDyCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one NaDyCl6 framework. In the NaDyCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent DyCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.70 Å. Dy3+ is bonded to six equivalent Cl1- atoms to form DyCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Dy–Cl bond lengths are 2.62 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Dy3+ atom.

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Materials Data on Na3NdCl6 by Materials Project

(Na)2NaNdCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one NaNdCl6 framework. In the NaNdCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent NdCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.71 Å. Nd3+ is bonded to six equivalent Cl1- atoms to form NdCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Nd–Cl bond lengths are 2.71 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Nd3+ atom.

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Materials Data on Na2HgAsCl6 by Materials Project

(Na)2HgAsCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one HgAsCl6 framework. In the HgAsCl6 framework, Hg2+ is bonded to six equivalent Cl1- atoms to form HgCl6 octahedra that share corners with six equivalent AsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Hg–Cl bond lengths are 2.79 Å. As2+ is bonded to six equivalent Cl1- atoms to form AsCl6 octahedra that share corners with six equivalent HgCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All As–Cl bond lengths are 2.51 Å. Cl1- is bonded in a linear geometry to one Hg2+ and one As2+ atom.

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Materials Data on Na2TlCuBr6 by Materials Project

(Na)2CuTlBr6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one CuTlBr6 framework. In the CuTlBr6 framework, Cu1+ is bonded to six equivalent Br1- atoms to form CuBr6 octahedra that share corners with six equivalent TlBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cu–Br bond lengths are 2.57 Å. Tl3+ is bonded to six equivalent Br1- atoms to form TlBr6 octahedra that share corners with six equivalent CuBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–Br bond lengths are 2.85 Å. Br1- is bonded in a linear geometry to one Cu1+ and one Tl3+ atom.

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Materials Data on H(WO3)4 by Materials Project

(WO3)8H2 is High-temperature superconductor-derived structured and crystallizes in the tetragonal I-42m space group. The structure is three-dimensional and consists of two dihydrogen molecules and one WO3 framework. In the WO3 framework, W+5.75+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of W–O bond distances ranging from 1.83–2.08 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent W+5.75+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent W+5.75+ atoms.

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Materials Data on CsK2SbCl6 by Materials Project

(K)2CsSbCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one CsSbCl6 framework. In the CsSbCl6 framework, Cs1+ is bonded to six equivalent Cl1- atoms to form CsCl6 octahedra that share corners with six equivalent SbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Cl bond lengths are 3.24 Å. Sb3+ is bonded to six equivalent Cl1- atoms to form SbCl6 octahedra that share corners with six equivalent CsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Cl bond lengths are 2.66 Å. Cl1- is bonded in a linear geometry to one Cs1+ and one Sb3+ atom.

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Materials Data on Na2InAgCl6 by Materials Project

(Na)2AgInCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one AgInCl6 framework. In the AgInCl6 framework, Ag1+ is bonded to six equivalent Cl1- atoms to form AgCl6 octahedra that share corners with six equivalent InCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ag–Cl bond lengths are 2.67 Å. In3+ is bonded to six equivalent Cl1- atoms to form InCl6 octahedra that share corners with six equivalent AgCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–Cl bond lengths are 2.54 Å. Cl1- is bonded in a linear geometry to one Ag1+ and one In3+ atom.

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Materials Data on FeSnO6 by Materials Project

FeSnO6 is High-temperature superconductor-derived structured and crystallizes in the cubic Pn-3m space group. The structure is three-dimensional. Fe is bonded to six equivalent O atoms to form FeO6 octahedra that share corners with six equivalent SnO6 octahedra. The corner-sharing octahedral tilt angles are 1°. All Fe–O bond lengths are 1.82 Å. Sn is bonded to six equivalent O atoms to form SnO6 octahedra that share corners with six equivalent FeO6 octahedra. The corner-sharing octahedral tilt angles are 1°. All Sn–O bond lengths are 2.03 Å. O is bonded in a linear geometry to one Fe and one Sn atom.

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